{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:QRCS2QCRJFOTQFDSGLYEKTMM33","short_pith_number":"pith:QRCS2QCR","schema_version":"1.0","canonical_sha256":"84452d4051495d38147232f0454d8cdeefdc3cd7887d27aadb01e52c8db5dd58","source":{"kind":"arxiv","id":"hep-lat/9710052","version":1},"attestation_state":"computed","paper":{"title":"Lattice Renormalization of Quark Operators","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Schiller, G. Schierholz, H. Oelrich, H. Perlt, M. Goeckeler, P. E. L. Rakow, R. Horsley","submitted_at":"1997-10-13T15:10:07Z","abstract_excerpt":"We have technically improved the non-perturbative renormalization method, proposed by Martinelli et al., by using quark momentum sources and sinks. Composite two-fermion operators up to three derivatives have been measured for Wilson fermions and Sheikholeslami-Wohlert improved fermions in the quenched approximation. The calculations are performed in the Landau gauge on 16^3x32 lattices at beta = 6.0 for 3 kappa values in each case. The improved sources greatly decrease the statistical noise. We extract and discuss here renormalization factors for local operators and moments of the structure f"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-lat/9710052","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1997-10-13T15:10:07Z","cross_cats_sorted":[],"title_canon_sha256":"ce7836e19282dfbf17bae653feea24c07b9fd31d536121539c63ebb5b4a55bc4","abstract_canon_sha256":"537850ba998099a1d0a9113efc97e17c61ee9eb7b147583fad63dbfd0e9b3f3c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:29:31.823537Z","signature_b64":"K9ifGwfDbxYSjV2oswHFDl76eGH2kNjkRe3ccRzKbSnKtIAfUpwklIQnxRlPQk2FohRNitz+fNAAHAyLUy4wCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84452d4051495d38147232f0454d8cdeefdc3cd7887d27aadb01e52c8db5dd58","last_reissued_at":"2026-07-04T15:29:31.823122Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:29:31.823122Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice Renormalization of Quark Operators","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Schiller, G. Schierholz, H. Oelrich, H. Perlt, M. Goeckeler, P. E. L. Rakow, R. Horsley","submitted_at":"1997-10-13T15:10:07Z","abstract_excerpt":"We have technically improved the non-perturbative renormalization method, proposed by Martinelli et al., by using quark momentum sources and sinks. Composite two-fermion operators up to three derivatives have been measured for Wilson fermions and Sheikholeslami-Wohlert improved fermions in the quenched approximation. The calculations are performed in the Landau gauge on 16^3x32 lattices at beta = 6.0 for 3 kappa values in each case. The improved sources greatly decrease the statistical noise. We extract and discuss here renormalization factors for local operators and moments of the structure f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9710052","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9710052/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9710052","created_at":"2026-07-04T15:29:31.823176+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9710052v1","created_at":"2026-07-04T15:29:31.823176+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9710052","created_at":"2026-07-04T15:29:31.823176+00:00"},{"alias_kind":"pith_short_12","alias_value":"QRCS2QCRJFOT","created_at":"2026-07-04T15:29:31.823176+00:00"},{"alias_kind":"pith_short_16","alias_value":"QRCS2QCRJFOTQFDS","created_at":"2026-07-04T15:29:31.823176+00:00"},{"alias_kind":"pith_short_8","alias_value":"QRCS2QCR","created_at":"2026-07-04T15:29:31.823176+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33","json":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33.json","graph_json":"https://pith.science/api/pith-number/QRCS2QCRJFOTQFDSGLYEKTMM33/graph.json","events_json":"https://pith.science/api/pith-number/QRCS2QCRJFOTQFDSGLYEKTMM33/events.json","paper":"https://pith.science/paper/QRCS2QCR"},"agent_actions":{"view_html":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33","download_json":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33.json","view_paper":"https://pith.science/paper/QRCS2QCR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9710052&json=true","fetch_graph":"https://pith.science/api/pith-number/QRCS2QCRJFOTQFDSGLYEKTMM33/graph.json","fetch_events":"https://pith.science/api/pith-number/QRCS2QCRJFOTQFDSGLYEKTMM33/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33/action/storage_attestation","attest_author":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33/action/author_attestation","sign_citation":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33/action/citation_signature","submit_replication":"https://pith.science/pith/QRCS2QCRJFOTQFDSGLYEKTMM33/action/replication_record"}},"created_at":"2026-07-04T15:29:31.823176+00:00","updated_at":"2026-07-04T15:29:31.823176+00:00"}